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QM’05 Budapest, HungaryHiroshi Masui (Univ. of Tsukuba) 1 Anisotropic Flow in  s NN = 200 GeV Cu+Cu and Au+Au collisions at RHIC - PHENIX Hiroshi Masui.

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Presentation on theme: "QM’05 Budapest, HungaryHiroshi Masui (Univ. of Tsukuba) 1 Anisotropic Flow in  s NN = 200 GeV Cu+Cu and Au+Au collisions at RHIC - PHENIX Hiroshi Masui."— Presentation transcript:

1 QM’05 Budapest, HungaryHiroshi Masui (Univ. of Tsukuba) 1 Anisotropic Flow in  s NN = 200 GeV Cu+Cu and Au+Au collisions at RHIC - PHENIX Hiroshi Masui for the PHENIX collaboration August 5, 2005 Quark Matter 2005

2 Hiroshi Masui (Univ. of Tsukuba) 2 QM’05 Budapest, Hungary Introduction Identified hadron v 2 Early thermalization Constituent quark scaling  Partonic collectivity Energy dependence Saturation of v 2 at RHIC 50 % increase from SPS PRL 91, 182301 PRL 94, 232302

3 Hiroshi Masui (Univ. of Tsukuba) 3 QM’05 Budapest, Hungary Motivation Anisotropic flow can be reasonably described with hydrodynamical model at RHIC. Hydrodynamics predict large v 2 and several scaling relations v 4 /(v 2 ) 2 scaling Eccentricity scaling Scaling with system size It is crucial to test these scaling in order to understand the system properties.

4 Hiroshi Masui (Univ. of Tsukuba) 4 QM’05 Budapest, Hungary Outline Recent results of event anisotropy at PHENIX v 4 for unidentified and identified hadrons in Au+Au Scaling ratio, v 4 /(v 2 ) 2 v 2 for identified hadrons in Au+Au Intermediate p T Charm,  System size dependence of v 2 Eccentricity scaling Summary

5 Hiroshi Masui (Univ. of Tsukuba) 5 QM’05 Budapest, Hungary Analysis method Event plane Beam-Beam Counter, |  | ~ 3 – 4. Large rapidity gap (  ~ 3)  could reduce non-flow contribution PID High resolution Time-of-Flight  /K separation ~ 3 GeV/c, K/p separation ~ 5 GeV/c Aerogel Cherenkov Counter Higher p T PID with combining EMC timing information Aerogel TOF BB

6 Hiroshi Masui (Univ. of Tsukuba) 6 QM’05 Budapest, Hungary Scaling of v 4

7 Hiroshi Masui (Univ. of Tsukuba) 7 QM’05 Budapest, Hungary v 4 {EP 2 } vs p T v 4 {EP 2 } v 4 with respect to the second harmonic BBC event plane. Very large v 2 at RHIC ! Hydro works. v 4 ~ (v 2 ) 2 (Ollitrault) v 4 /(v 2 ) 2 ~ 1.5, flat. consistent with STAR results (1.2).

8 Hiroshi Masui (Univ. of Tsukuba) 8 QM’05 Budapest, Hungary PID v 4 {EP 2 } v 4 measurement for identified hadrons. How about the scaling for identified hadrons ?

9 Hiroshi Masui (Univ. of Tsukuba) 9 QM’05 Budapest, Hungary v 4 /(v 2 ) 2 scaling ratio Meson, baryon comparison

10 Hiroshi Masui (Univ. of Tsukuba) 10 QM’05 Budapest, Hungary v 4 /(v 2 ) 2 scaling ratio Meson, baryon comparison Simple coalescence calculation, meson ~ 3/4, baryon ~ 2/3 (Kolb et al, PRC 69, 051901)  underestimate

11 Hiroshi Masui (Univ. of Tsukuba) 11 QM’05 Budapest, Hungary v 4 /(v 2 ) 2 scaling ratio Meson, baryon comparison Simple coalescence calculation, meson ~ 3/4, baryon ~ 2/3 (Kolb et al, PRC 69, 051901)  underestimate Data seems to be scaled by 1.5

12 Hiroshi Masui (Univ. of Tsukuba) 12 QM’05 Budapest, Hungary Identified hadron v 2

13 Hiroshi Masui (Univ. of Tsukuba) 13 QM’05 Budapest, Hungary What’s new ? Run2002 Au+Au at  s NN = 200 GeV Measured at High resolution Time-of- Flight counter.  /K/p v 2  /K ~ 3 GeV/c p ~ 4 GeV/c PRL 91, 182301

14 Hiroshi Masui (Univ. of Tsukuba) 14 QM’05 Budapest, Hungary What’s new ? High statistics in Run2004 Au+Au at  s NN = 200 GeV Extend p T for  /K/p with simultaneous 3 gaussian fitting to mass square distribution , p p T < 5 GeV/c K, p T < 4 GeV/c

15 Hiroshi Masui (Univ. of Tsukuba) 15 QM’05 Budapest, Hungary Aerogel Aerogel can cover much higher p T. Pion is quite consistent with reco model. Proton seems to decrease for p T = 4 – 5 GeV/c Similar trend in TOF. Need further study at higher p T

16 Hiroshi Masui (Univ. of Tsukuba) 16 QM’05 Budapest, Hungary All identified particles Charm has strong flow !  thermalization  is also flowing !  partonic collectivity  0 : D. L. Winter (talk), K. Miki (poster) n.p. electron S. A. Butsyk (talk), S. Sakai (poster)  : D. Pal (talk)

17 Hiroshi Masui (Univ. of Tsukuba) 17 QM’05 Budapest, Hungary System size dependence Au+Au vs Cu+Cu

18 Hiroshi Masui (Univ. of Tsukuba) 18 QM’05 Budapest, Hungary Linear scaling ? AMPT An approximate linear scaling with the system size. v 2 (Cu+Cu) ~ 0.3 * v 2 (Au+Au)

19 Hiroshi Masui (Univ. of Tsukuba) 19 QM’05 Budapest, Hungary Linear scaling ? AMPT An approximate linear scaling with the system size. v 2 (Cu+Cu) ~ 0.3 * v 2 (Au+Au) First results of v 2 in smaller system, Cu+Cu < 10 % of total data v 2 seems to NOT scale by system size linearly. v 2 (Cu) ~ 0.84 * v 2 (Au)

20 Hiroshi Masui (Univ. of Tsukuba) 20 QM’05 Budapest, Hungary Eccentricity scaling v 2 (integral) ~  v 2 (p T )/v 2 (integral) Reduce systematic errors related to eccentricity calculation and event plane resolution. Scaling would be roughly independent of the system size  Suggest that hydrodynamical regime is reached in central - mid-central Cu+Cu collisions. See poster by A. Taranenko

21 Hiroshi Masui (Univ. of Tsukuba) 21 QM’05 Budapest, Hungary Constituent quark scaling Smaller v 2 in Cu+Cu Similar trend for identified hadron v 2 in Cu+Cu compared to that in Au+Au Constituent quark scaling in Cu+Cu ? Need much more statistics

22 Hiroshi Masui (Univ. of Tsukuba) 22 QM’05 Budapest, Hungary Summary v 4 scaling v 4 /(v 2 ) 2 scaling ratio ~ 1.5 for both unidentified and identified hadrons. larger by factor 2 – 3 from model prediction. Identified hadron v 2 Proton v 2 seems to decrease around p T ~ 4 – 5 GeV/c. Further study need to be done at higher p T. Charm,  has a strong flow ! Scaling with system size The scaling of v 2 with system size seems to not linear. Eccentricity scaling would be roughly independent of the system size Suggest that hydro regime is reached in central – mid-central Cu+Cu collisions. Similar tendency of identified hadron v 2 in Cu+Cu compared to Au+Au is observed.

23 Hiroshi Masui (Univ. of Tsukuba) 23 QM’05 Budapest, Hungary Flow talks, posters Talks D. L. Winter (  0, charged hadron at high p T ) Parallel1, 3a (Aug. 5, Fri.) PHENIX measurement of particle yield at high p T with respect to the reaction plane in Au+Au collisions at  s NN = 200 GeV D. Pal (  meson) Parallel1, 1b (Aug. 5, Fri.) Nuclear Modifications and elliptic flow measurements for  mesons at  s NN = 200 GeV d+Au and Au+Au collisions by PHENIX Posters B. E. Norman (v 1, v 2 at MVD) Poster1, 49 (Aug. 4 – 5) Azimuthal anisotropy at intermediate rapidity in  s NN = 200 GeV Au-Au collisions using the PHENIX MVD S. Sakai (electron v 2 ) Poster1, 51 (Aug. 4 – 5) The azimuthal anisotropy of electrons from heavy flavor decays in  s NN = 200 GeV Au-Au collisions by PHENIX A. Taranenko (identified hadron v 2 in Au+Au and Cu+Cu) Poster1, 52 (Aug. 4 – 5) Scaling properties of azimuthal anisotropy at RHIC K. Miki (  0, photon v 2 ) Poster1, 192 (Aug. 4 – 5) Measurement of inclusive photon and direct photon v 2 in  s NN = 200 GeV Au-Au collision with PHENIX experiment at RHIC M. Konno (Aerogel v 2 ) Poster1, 222 (Aug 6 – 8) Identified charged hadron production at high pT in  s NN = 200 GeV Au+Au collisions

24 Hiroshi Masui (Univ. of Tsukuba) 24 QM’05 Budapest, Hungary

25 Hiroshi Masui (Univ. of Tsukuba) 25 QM’05 Budapest, Hungary Back up

26 Hiroshi Masui (Univ. of Tsukuba) 26 QM’05 Budapest, Hungary Event plane Method Determine event plane at Beam-Beam Counter (|  | ~ 3 – 4) Measure event anisotropy in PHENIX central arm (|  |<0.35) Large rapidity gap (  ~ 3)  Reduce non-flow effect

27 Hiroshi Masui (Univ. of Tsukuba) 27 QM’05 Budapest, Hungary Charged Particle identification at PHENIX High resolution Time-of-flight  /K separation ~ 3 GeV/c, K/p separation ~ 5 GeV/c

28 Hiroshi Masui (Univ. of Tsukuba) 28 QM’05 Budapest, Hungary Charged Particle identification at PHENIX High resolution Time-of-flight  /K separation ~ 3 GeV/c, K/p separation ~ 5 GeV/c Aerogel counter  Threshold type Cherenkov counter Combined Aerogel + TOF (EMC)  PID in higher p T.

29 Hiroshi Masui (Univ. of Tsukuba) 29 QM’05 Budapest, Hungary v 1 at MVD v 1 measurement at PHENIX MVD with respect to the 1 st harmonic BBC event plane. Cover intermediate rapidity between PHENIX central arm and BBC, |  | ~ 1 – 3 See Poster by B. E. Norman

30 Hiroshi Masui (Univ. of Tsukuba) 30 QM’05 Budapest, Hungary v 2 at MVD

31 Hiroshi Masui (Univ. of Tsukuba) 31 QM’05 Budapest, Hungary v 2 vs p T, minimum bias

32 Hiroshi Masui (Univ. of Tsukuba) 32 QM’05 Budapest, Hungary Centrality depedence

33 Hiroshi Masui (Univ. of Tsukuba) 33 QM’05 Budapest, Hungary Constituent quark scaling

34 Hiroshi Masui (Univ. of Tsukuba) 34 QM’05 Budapest, Hungary PID v2 in Cu+Cu

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